NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.C.Awes Found 43 matches. 2013AG03 Nucl.Phys. A898, 14 (2013) M.M.Aggarwal, Z.Ahammed, A.L.S.Angelis, V.Antonenko, V.Arefiev, V.Astakhov, V.Avdeitchikov, T.C.Awes, P.V.K.S.Baba, S.K.Badyal, S.Bathe, B.Batiounia, C.Baumann, T.Bernier, K.B.Bhalla, V.S.Bhatia, C.Blume, D.Bucher, H.Busching, L.Carlen, S.Chattopadhyay, M.P.Decowski, H.Delagrange, P.Donni, M.R.Dutta Majumdar, K.El Chenawi, A.K.Dubey, K.Enosawa, S.Fokin, V.Frolov, M.S.Ganti, S.Garpman, O.Gavrishchuk, F.J.M.Geurts, T.K.Ghosh, R.Glasow, B.Guskov, H.A.Gustafsson, H.H.Gutbrod, I.Hrivnacova, M.Ippolitov, H.Kalechofsky, R.Kamermans, K.Karadjev, K.Karpio, B.W.Kolb, I.Kosarev, I.Koutcheryaev, A.Kugler, P.Kulinich, M.Kurata, A.Lebedev, H.Lohner, L.Luquin, D.P.Mahapatra, V.Manko, M.Martin, G.Martinez, A.Maximov, Y.Miake, G.C.Mishra, B.Mohanty, M.-J.Mora, D.Morrison, T.Mukhanova, D.S.Mukhopadhyay, H.Naef, B.K.Nandi, S.K.Nayak, T.K.Nayak, A.Nianine, V.Nikitine, S.Nikolaev, P.Nilsson, S.Nishimura, P.Nomokonov, J.Nystrand, A.Oskarsson, I.Otterlund, S.Pavliouk, T.Peitzmann, D.Peressounko, V.Petracek, S.C.Phatak, W.Pinganaud, F.Plasil, M.L.Purschke, J.Rak, M.Rammler, R.Raniwala, S.Raniwala, N.K.Rao, F.Retier, K.Reygers, G.Roland, L.Rosselet, I.Roufanov, C.Roy, J.M.Rubio, S.S.Sambyal, R.Santo, S.Sato, H.Schlagheck, H.-R.Schmidt, Y.Schutz, G.Shabratova, T.H.Shah, I.Sibiriak, T.Siemiarczuk, D.Silvermyr, B.C.Sinha, N.Slavine, K.Soderstrom, G.Sood, S.P.Sorensen, P.Stankus, G.Stefanek, P.Steinberg, E.Stenlund, M.Sumbera, T.Svensson, A.Tsvetkov, L.Tykarski, E.C.v.d.Pijll, N.v.Eijndhoven, G.J.v.Nieuwenhuizen, A.Vinogradov, Y.P.Viyogi, A.Vodopianov, S.Voros, B.Wyslouch, G.R.Young Photon and η production in p + Pb and p + C collisions at √ sNN=17.4 GeV
doi: 10.1016/j.nuclphysa.2012.11.010
2007BE15 Phys.Rev. A 75, 034501 (2007) S.Berridge, W.Bugg, Yu.Efremenko, R.Gearhart, S.Ovchinnikov, T.C.Awes, V.Cianciolo, Yu.I.Davydov, T.Numao, J.M.Poutissou π- nuclear capture ratio on hydrogen and oxygen in water NUCLEAR REACTIONS H, C, O(π-, X), E=70 MeV/c; measured pion capture ratio on H2O and CH2.
doi: 10.1103/PhysRevA.75.034501
2006AW01 Pramana 67, 915 (2006) Status of the quark gluon plasma search
doi: 10.1007/s12043-006-0102-1
2004AW01 Acta Phys.Pol. B35, 1081 (2004) T.C.Awes, for the PHENIX Collaboration Recent Results on High pT Particle Production from the PHENIX Experiment NUCLEAR REACTIONS 197Au(d, X), (197Au, X), E(cm)=200 GeV/nucleon; measured particles transverse momentum; deduced suppression factor.
2004GA39 J.Phys.(London) G30, S1013 (2004) C.Gale, T.C.Awes, R.J.Fries, D.K.Srivastava The electromagnetic signature of jets NUCLEAR REACTIONS Pb(Pb, X), E(cm)=200, 5500 GeV/nucleon; 197Au(197Au, X), E(cm)=200 GeV/nucleon; calculated dilepton spectra, contribution from jet-plasma interactions.
doi: 10.1088/0954-3899/30/8/049
2003SR02 Phys.Rev. C 67, 054904 (2003) D.K.Srivastava, C.Gale, T.C.Awes Dilepton-tagged jets in relativistic nucleus-nucleus collisions: A case study NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=200 GeV/nucleon; Pb(Pb, X), E(cm)=5500 GeV/nucleon; calculated dilepton-tagged jet event rates, associated spectra, rapidity correlations.
doi: 10.1103/PhysRevC.67.054904
1998AW01 Nucl.Phys. A630, 499c (1998) T.C.Awes, for the WA98 Collaboration Collective Flow as a Probe of Heavy-Ion Reaction Dynamics
doi: 10.1016/S0375-9474(97)00789-6
1997KA62 Z.Phys. C74, 587 (1997) K.H.Kampert, T.C.Awes, P.Stankus, H.H.Gutbrod, V.Manko, T.Peitzmann, R.Santo Comment on Search for Direct Photons from S-Au Collisions at GeV/Nucleon by the CERES Collaboration NUCLEAR REACTIONS 197Au(S, X), E=high; analyzed previous analysis; deduced new direct photon yield uncertainty. CERES experiment data.
doi: 10.1007/s002880050422
1996AW02 Phys.Lett. 381B, 29 (1996) T.C.Awes, and the WA80 Collaboration Azimuthal Correlations in the Target Fragmentation Region of High Energy Nuclear Collisions NUCLEAR REACTIONS 197Au(p, X), (O, X), (S, X), E at 200 GeV/c; measured proton, pion pseudorapidity distributions, their azimuthal correlations; deduced strong rescattering phenomena role. Other reactions also studied.
doi: 10.1016/0370-2693(96)00601-6
1996SR04 Phys.Lett. 387B, 21 (1996) D.K.Srivastava, B.Sinha, T.C.Awes Photon Pairs from Relativistic Heavy Ion Collisions and the Quark Hadron Phase Transition NUCLEAR REACTIONS 197Au(S, X), E=high; calculated photon pair invariant mass distribution from q(q-bar), π+π--annihilation, relativistic collisions. Hydrodynamics, transverse expansion.
doi: 10.1016/0370-2693(96)00977-X
1995AW01 Nucl.Phys. A590, 81c (1995) T.C.Awes, and the WA80 Collaboration Search for Direct Photon Production in 200 A GeV S + Au Reactions: A status report NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; measured single photon production σ, neutral π0, η production σ; deduced hadronic decays evidence.
doi: 10.1016/0375-9474(95)00227-R
1995AW02 Z.Phys. C65, 207 (1995) T.C.Awes, and the WA80 Collaboration Two-Proton Correlations in the Target Fragmentation Region of Nuclear Collisions at 200 A GeV NUCLEAR REACTIONS C, Cu, Ag, 197Au(p, X), (16O, X), 27Al, 197Au(32S, X), E=200 GeV/nucleon; measured pp-correlation; deduced radius parameters, target fragmentation features.
1990PE08 Phys.Rev. C42, 1489 (1990) V.Penumetcha, G.A.Petitt, T.C.Awes, J.R.Beene, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.P.Sorensen Charge and Mass Distributions in Strongly Damped Reactions of 58Ni + 165Ho at 16 MeV/Nucleon NUCLEAR REACTIONS 165Ho(58Ni, X), E=16 MeV/nucleon; measured fragment charge, mass distributions; deduced proton transfer role in reaction mechanism. Statistical evaporation.
doi: 10.1103/PhysRevC.42.1489
1989PE07 Phys.Rev. C40, 692 (1989) G.A.Petitt, C.Butler, V.Penumetcha, T.C.Awes, J.R.Beene, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.P.Sorensen Neutron Emission from Products of Strongly Damped Reactions 58Ni + 165Ho at 930 MeV NUCLEAR REACTIONS 165Ho(58Ni, X), E=930 MeV; measured product neutron emission spectra, n(fragment)-coin; deduced model parameters. Moving source fits.
doi: 10.1103/PhysRevC.40.692
1988AW01 Phys.Rev.Lett. 61, 2665 (1988) T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.Pratt, Z.Chen, C.K.Gelbke, W.G.Lynch, J.Pochodzalla, H.M.Xu Extended Emission Sources Observed via Two-Proton Correlations NUCLEAR REACTIONS Ag(32S, pX), E=715 MeV; measured pp-correlation; deduced emission mechanism.
doi: 10.1103/PhysRevLett.61.2665
1988VA05 Phys.Rev. C37, 1301 (1988) R.Vandenbosch, R.C.Connolly, S.Gil, D.D.Leach, T.C.Awes, S.Sorensen, C.Y.Wu Light-Particle Multiplicity Accompanying Projectile Breakup at 20 MeV/Nucleon NUCLEAR REACTIONS 181Ta(35Cl, X), (35Cl, αX), E=700 MeV; measured p(fragment)(fragment)-, α(fragment)(fragment)-coin; deduced α-, p-multiplicity.
doi: 10.1103/PhysRevC.37.1301
1987GA01 Phys.Rev. C35, 579 (1987) A.Gavron, A.Gayer, J.Boissevain, H.C.Britt, T.C.Awes, J.R.Beene, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, G.A.Petitt, C.Butler Neutron Emission in the Fissioning 158Er Composite System NUCLEAR REACTIONS 142Nd(16O, F), E=207 MeV; 134Ba(24Mg, F), 126Te(32S, F), E=180 MeV; 108Pd(50Ti, F), E=216 MeV; measured fission (fragment)n-coin. 158Er deduced fissioning characteristics. NE213 scintillators, tof. Model calculations.
doi: 10.1103/PhysRevC.35.579
1986AL09 Phys.Lett. 173B, 392 (1986) N.Alamanos, P.Braun-Munzinger, R.F.Freifelder, P.Paul, J.Stachel, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young Observation of High Energy Electromagnetic Dipole Radiation in 14N + Ni Reactions at E(lab)/A = 35 MeV NUCLEAR REACTIONS Ni(14N, X), E=35 MeV/nucleon; measured σ(θ, Eγ), γ(θ); deduced high energy dipole radiation.
doi: 10.1016/0370-2693(86)90401-6
1986CH27 Phys.Rev. C34, 858 (1986) C.B.Chitwood, D.J.Fields, C.K.Gelbke, D.R.Klesch, W.G.Lynch, M.B.Tsang, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson, G.R.Young Light Particle Emission in 16O-Induced Reactions on 12C, 27Al, and 197Au at E/A = 25 MeV NUCLEAR REACTIONS 12C, 27Al, 197Au(16O, pX), (16O, dX), (16O, tX), E=400 MeV; measured inclusive σ(Ep, θp), σ(Ed, θd), σ(Et, θt); deduced light particle emission mechanism.
doi: 10.1103/PhysRevC.34.858
1986FI10 Phys.Rev. C34, 536 (1986) D.J.Fields, W.G.Lynch, T.K.Nayak, M.B.Tsang, C.B.Chitwood, C.K.Gelbke, R.Morse, J.Wilczynski, T.C.Awes, R.L.Ferguson, F.Plasil, F.E.Obenshain, G.R.Young Coincidence Measurements of Intermediate Mass Fragments Produced in 32S-Induced Reactions on Ag at E/A = 22.5 MeV NUCLEAR REACTIONS Ag(32S, X), E=720 MeV; measured σ(E, θ), σ(E1, θ1, E2, θ2), target residue velocity spectra, two particle correlations for Z=3-24; deduced light particle, fragment multiplicities, momentum transfer, energy loss.
doi: 10.1103/PhysRevC.34.536
1986ST03 Phys.Rev. C33, 1420 (1986) J.Stachel, P.Braun-Munzinger, R.H.Freifelder, P.Paul, S.Sen, P.DeYoung, P.H.Zhang, T.C.Awes, F.E.Obenshain, F.Plasil, G.R.Young, R.Fox, R.Ronningen Pion Production: A probe for coherence in medium-energy heavy-ion collisions NUCLEAR REACTIONS Ni, 27Al(14N, π0X), E=35 MeV/nucleon; 27Al, Ni(16O, π0X), E=25 MeV/nucleon; measured inclusive pion production σ(θ(π), E(π)), invariant pion mass; deduced pion production, reabsorption mechanisms.
doi: 10.1103/PhysRevC.33.1420
1985AW01 Phys.Rev.Lett. 55, 1062 (1985) T.C.Awes, R.L.Ferguson, R.Novotny, F.E.Obenshain, F.Plasil, V.Rauch, G.R.Young, H.Sann Fission Decay of Reaction Products with A ≤ 150 NUCLEAR REACTIONS 58Ni(58Ni, X), E=15.3 MeV/nucleon; measured (fragment)(fragment)-coin; deduced heavy fragment decay characteristics, fission probability vs excitation energy.
doi: 10.1103/PhysRevLett.55.1062
1985BE02 Phys.Rev.Lett. 54, 402 (1985) M.A.Bernstein, W.A.Friedman, W.G.Lynch, C.B.Chitwood, D.J.Fields, C.K.Gelbke, M.B.Tsang, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson, G.R.Young Statistical Emisssion of 2He from Highly Excited Nuclear Systems NUCLEAR REACTIONS 12C, 27Al(16O, 2pX), E=400 MeV; measured σ(θp1, θp2). 28Si, 43Sc deduced particle unstable nuclei decay channel importance.
doi: 10.1103/PhysRevLett.54.402
1985CH02 Phys.Rev.Lett. 54, 302 (1985) C.B.Chitwood, J.Aichelin, D.H.Boal, G.Bertsch, D.J.Fields, C.K.Gelbke, W.G.Lynch, M.B.Tsang, J.C.Shillcock, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson, G.R.Young Final-State Interactions between Noncompound Light Particles for 16O-Induced Reactions on 197Au at E/A = 25 MeV NUCLEAR REACTIONS 197Au(16O, 2d), (16O, 2t), (16O, 2p), E=25 MeV/nucleon; measured (particle-particle) correlation function; deduced final state interactions role.
doi: 10.1103/PhysRevLett.54.302
1984AW01 Phys.Rev.Lett. 52, 251 (1984) T.C.Awes, R.L.Ferguson, R.Novotny, F.E.Obenshain, F.Plasil, S.Pontoppidan, V.Rauch, G.R.Young, H.Sann Energy Division in Damped Reactions NUCLEAR REACTIONS 58Ni, 197Au(58Ni, X), E=15.3 MeV/nucleon; measured fragment yield vs Z, kinetic energies; deduced reaction mechnism. 165Ho(56Fe, X), E=8.5 MeV/nucleon; analyzed data; deduced charge, neutron number centroids, average fragment multiplicity vs energy loss.
doi: 10.1103/PhysRevLett.52.251
1984GA30 Phys.Rev. C30, 1550 (1984) A.Gavron, J.Boissevain, H.C.Britt, K.Eskola, P.Eskola, M.M.Fowler, H.Ohm, J.B.Wilhelmy, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, G.R.Young, S.Wald Fission Cross Sections up to 20 MeV/Nucleon NUCLEAR REACTIONS, ICPND 174Yb, 198Pt, 238U(12C, F), E=95-291 MeV; 142Nd, 170Er, 192Os, 238U(16O, F), E=140-315 MeV; 126Te, 144Nd, 238U(32S, F), E=350, 500, 700; 96Zr, 116Cd, 238U(58Ni, F), E=352, 875 MeV; measured fission σ(E), fragment σ(θ) anisotropy; deduced incomplete fusion reaction role.
doi: 10.1103/PhysRevC.30.1550
1984MU21 Phys.Rev.Lett. 53, 1543 (1984) M.J.Murphy, S.Gil, M.N.Harakeh, A.Ray, A.G.Seamster, R.Vandenbosch, T.C.Awes Time Scale for Projectile Breakup into Coincident Heavy Fragments NUCLEAR REACTIONS Ta(35Cl, X), E=680 MeV; measured (fragment)(fragment)-coin for Z=3-8; deduced sequential projectile breakup mechanism.
doi: 10.1103/PhysRevLett.53.1543
1984PL01 Phys.Rev. C29, 1145 (1984) F.Plasil, T.C.Awes, B.Cheynis, D.Drain, R.L.Ferguson, F.E.Obenshain, A.J.Sierk, S.G.Steadman, G.R.Young Angular-Momentum-Dependent Fission Barriers in the Rare-Earth Region NUCLEAR REACTIONS, ICPND 169Tm(12C, X), E=78.2, 100.8, 122.6 MeV; 159Tb(22Ne, X), E=113, 130, 161.5 MeV; measured evaporation residue production σ. 133Cs(20Ne, F), 141Pr, 169Tm(12C, F), 159Tb(22Ne, F), E not given; calculated fission σ vs excitation function. 153Tb, 181Re deduced level density parameters ratio (a(F)/a(ν)). Angular momentum dependent fission barriers, rotating liquid drop, rotating finite-range models.
doi: 10.1103/PhysRevC.29.1145
1984TS07 Phys.Lett. 148B, 265 (1984) M.B.Tsang, W.G.Lynch, C.B.Chitwood, D.J.Fields, D.R.Klesch, C.K.Gelbke, G.R.Young, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson Azimuthal Correlations between Light Particles Emitted in 16O Induced Reactions on 12C and 197Au at 400 MeV NUCLEAR REACTIONS 12C, 197Au(16O, X), E=400 MeV; measured σ(fragment θ, t), (fragment)(fragment)(θ) for pp-, pd-, pt-, dd-, dt-pairs; deduced reaction mechanism.
doi: 10.1016/0370-2693(84)90085-6
1983LY05 Phys.Rev.Lett. 51, 1850 (1983) W.G.Lynch, C.B.Chitwood, M.B.Tsang, D.J.Fields, D.R.Klesch, C.K.Gelbke, G.R.Young, T.C.Awes, R.L.Ferguson, F.E.Obenshain, F.Plasil, R.L.Robinson, A.D.Panagiotou Formation and Decay of a Localized Region of High Excitation in Heavy-Ion-Induced Reactions NUCLEAR REACTIONS 197Au(16O, 2pX), E=400 MeV; measured pp-correlation; deduced localized proton emission.
doi: 10.1103/PhysRevLett.51.1850
1983VA23 Phys.Rev. C28, 2022 (1983) J.van der Plicht, H.C.Britt, M.M.Fowler, Z.Fraenkel, A.Gavron, J.B.Wilhelmy, F.Plasil, T.C.Awes, G.R.Young Fission of Polonium, Osmium, and Erbium Composite Systems NUCLEAR REACTIONS, ICPND 174Yb(16O, F), E=10 MeV/nucleon; 142Nd(16O, F), E=95-140 MeV; 134Ba(24Mg, F), E=120-180 MeV; 126Te(32S, F), E=150-220 MeV; 94Zr(64Ni, F), E=250, 270, 290 MeV; 177Hf(9Be, F), E=64-84 MeV; 174Yb(12C, F), E=65-120 MeV; 170Er(16O, F), E=80-150 MeV; 160Gd(26Mg, F), E=120-170 MeV; 198Pt(12C, F), E=55-120 MeV; 192Os(16O, F), E=78-150 MeV; 188Os(16O, F), (18O, F), E=80-140 MeV; measured fission σ(E). 158Er, 186Os, 210Po deduced fission barrier mass, angular momentum dependences.
doi: 10.1103/PhysRevC.28.2022
1982AW01 Phys.Rev. C25, 2361 (1982) T.C.Awes, S.Saini, G.Poggi, C.K.Gelbke, D.Cha, R.Legrain, G.D.Westfall Light Particle Emission in 16O-Induced Reactions at 140, 215, and 310 MeV NUCLEAR REACTIONS 27Al, 197Au(16O, p), (16O, d), (16O, t), (16O, α), E=140, 215, 310 MeV; 90Zr(16O, p), (16O, d), (16O, t), (16O, α), E=215, 310 MeV; measured σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θα, Eα); deduced emission mechanism. Moving source analysis, precompound, knockout, coalescence models.
doi: 10.1103/PhysRevC.25.2361
1982VI01 Phys.Rev. C26, 178 (1982) V.E.Viola, Jr., B.B.Back, K.L.Wolf, T.C.Awes, C.K.Gelbke, H.Breuer Linear Momentum Transfer in Nonrelativistic Nucleus-Nucleus Collisions NUCLEAR REACTIONS, Fission 238U(16O, F), E=140, 315 MeV; measured (fragment)(fragment)(θ); deduced linear momentum transfer distribution, complete fusion probabilities, J(critical), reaction mechanism.
doi: 10.1103/PhysRevC.26.178
1981AW01 Phys.Rev. C24, 89 (1981) T.C.Awes, G.Poggi, C.K.Gelbke, B.B.Back, B.G.Glagola, H.Breuer, V.E.Viola, Jr. Precompound Emission of Light Particles in the Reaction 16O + 238U at 20 MeV/Nucleon NUCLEAR REACTIONS, Fission 238U(16O, pF), (16O, dF), (16O, tF), (16O, αF), E=315 MeV; measured σ(Ep, θ), σ(Ed, θ), σ(Et, θ), σ(Eα, θ), (fragment)(fragment)(θ). Hot spot, moving source, coalescence models.
doi: 10.1103/PhysRevC.24.89
1981AW02 Phys.Lett. 103B, 417 (1981) T.C.Awes, G.Poggi, S.Saini, C.K.Gelbke, R.Legrain, G.D.Westfall Trends of Light Particle Spectra Observed in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 197Au, 27Al, 90Zr(16O, p), (16O, d), (16O, t), E=140, 215, 310 MeV; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et). Moving thermal source analysis.
doi: 10.1016/0370-2693(81)90073-3
1981BA11 Phys.Rev. C23, 1105 (1981) B.B.Back, A.C.Shotter, T.J.M.Symons, A.Bice, C.K.Gelbke, T.C.Awes, D.K.Scott Fission of 238U Induced by Inelastic Scattering of 120 MeV α Particles NUCLEAR REACTIONS, Fission 238U(α, α'F), E=120 MeV; measured total kinetic energy, fragment mass distributions vs excitation energy. Double energy method. Static scission point model.
doi: 10.1103/PhysRevC.23.1105
1981KA30 Phys.Lett. 104B, 434 (1981) J.Kasagi, S.Saini, T.C.Awes, A.Galonsky, C.K.Gelbke, G.Poggi, D.K.Scott, K.L.Wolf, R.L.Legrain Comparison of Non-Compound Neutron and Proton Emission in 16O Induced Reactions on 238U at 310 MeV NUCLEAR REACTIONS, Fission 238U(16O, nF), (16O, pF), E=310 MeV; measured σ(E, θ) vs neutron, proton number, n(fragment)-, p(fragment)-coin. Coalescence model.
doi: 10.1016/0370-2693(81)90509-8
1980AW01 Phys.Rev.Lett. 45, 513 (1980) T.C.Awes, C.K.Gelbke, G.Poggi, B.B.Back, B.Glagola, H.Breuer, V.E.Viola, Jr., T.J.M.Symons Coalescence of Light Paricles in the Reaction 16O+238U at 315 MeV NUCLEAR REACTIONS, Fission 238U(16O, pF), (16O, dF), (16O, tF), E=315 MeV; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et). Coulomb-modified coalescence model.
doi: 10.1103/PhysRevLett.45.513
1980BA41 Phys.Rev. C22, 1927 (1980) B.B.Back, K.L.Wolf, A.C.Mignerey, C.K.Gelbke, T.C.Awes, H.Breuer, V.E.Viola, Jr., P.Dyer Correlated Fission Fragments Emitted in the Reaction of 16O on 238U at 20 MeV/Nucleon NUCLEAR REACTIONS, Fission 238U(16O, pF), (16O, dF), (16O, tF), (16O, αF), E=315 MeV; measured p(fragment)-, d(fragment)-, t(fragment)-, α(fragment)-coin, σ(Ep), σ(Ed), σ(Et), σ(Eα); deduced missing momentum, fragment mass distribution, reaction mechanisms. Kinematic analysis.
doi: 10.1103/PhysRevC.22.1927
1979AW01 Phys.Lett. 87B, 43 (1979) T.C.Awes, C.K.Gelbke, B.B.Back, A.C.Mignerey, K.L.Wolf, P.Dyer, H.Breuer, V.E.Viola, Jr. Light Particle Spectra Observed in Central and Peripheral Collisions of 16O + 238U at 20 MeV/Nucleon NUCLEAR REACTIONS 238U(16O, pX), (16O, dX), (16O, tX), (16O, αX), E=315 MeV; measured light-particle spectra, σ(θ(fragment)).
doi: 10.1016/0370-2693(79)90013-3
1979DY01 Phys.Rev.Lett. 42, 560 (1979) P.Dyer, T.C.Awes, C.K.Gelbke, B.B.Back, A.Mignerey, K.L.Wolf, H.Breuer, V.E.Viola, Jr., W.G.Meyer Incomplete Momentum Transfer in Peripheral Heavy-Ion Collisions at 20 MeV/Nucleon NUCLEAR REACTIONS 238U(16O, XF), E=315 MeV; measured XF-coin; deduced incomplete momentum transfer.
doi: 10.1103/PhysRevLett.42.560
1979SH12 Phys.Rev.Lett. 43, 569 (1979) A.C.Shotter, C.K.Gelbke, T.C.Awes, B.B.Back, J.Mahoney, T.J.M.Symons, D.K.Scott Observation of Isoscalar Giant-Resonance Structure in the Fission of 238U Following Inelastic Scattering of 6Li NUCLEAR REACTIONS 238U(6Li, 6Li'F), E=150 MeV; measured σ(E(6Li')), 6Li'F-coin. 238U deduced isoscalar giant resonance structure.
doi: 10.1103/PhysRevLett.43.569
1979WE10 Phys.Rev.Lett. 43, 1859 (1979) G.D.Westfall, T.J.M.Symons, D.E.Greiner, H.H.Heckman, P.J.Lindstrom, J.Mahoney, A.C.Shotter, D.K.Scott, H.J.Crawford, C.McParland, T.C.Awes, C.K.Gelbke, J.M.Kidd Production of Neutron-Rich Nuclides by Fragmentation of 212 MeV/amu 48Ca NUCLEAR REACTIONS Be(48Ca, X)22N/26F/33Al/34Al/37Si/38Si/39Si/40P/41P/42P/41S/42S/43S/44S/44Cl/45Cl/21Na/22Na/23Na/24Na/25Na/26Na/27Na/28Na/29Na/30Na/31Na/32Na/33Na/34Na, E=212 MeV/nucleon; measured production σ. Thick target.
doi: 10.1103/PhysRevLett.43.1859
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